JP5523787B2 - Wafer defect detection system with moving lens multi-beam scanner - Google Patents

Description

  [01] The present invention relates to a wafer defect detection system that illuminates a wafer under analysis and uses a scanned laser beam to identify defects by analysis of reflected or transmitted light. In particular, the present invention relates to a scanner system using multiple beams that simultaneously illuminate a sample, such as a wafer, reticle, mask, etc., under inspection, and generate corresponding reflected or transmitted beams detected simultaneously.

  [02] As part of the quality assurance process in the semiconductor manufacturing process, various systems are used to automatically inspect semiconductor wafers to detect defects, particles, and / or patterns on the wafer surface . It is the goal of current inspection systems to have high resolution and high contrast imaging to provide the required reliability and accuracy in submicron semiconductor manufacturing processes. However, it is also important to have a high-speed process that allows a large amount of throughput so that the quality assurance process does not hinder progress during wafer production. Therefore, what must be used in an optical inspection system are shorter wavelengths, higher numerical aperture optics, and high density image capture technology, fast enough to meet the desired product throughput requirements, Data from such a system can be processed.

  [03] Conventional imaging architectures currently used in wafer inspection systems utilize a single spot scanning laser for high speed imaging. However, the data rates achievable with such an architecture are limited by physical constraints, applicable optics, and associated detection devices that result from speed and quality limitations of a single laser beam. For example, a single laser acting as a point source is focused on a spot on the object under inspection, scans through the surface of the object, and is stationary or moved on a stage mechanism in conjunction with the scan Good. The reflected light from the object is then imaged by a detector to produce pixel data from the scanning process. The detector may be a CCD array, the individual elements of which are arranged to receive the reflected light as the beam is scanned and sequentially read out, as is conventional. High resolution may be obtained from illumination of such point light sources, but if each point in the region needs to be scanned to construct a visible image, the system will be limited in throughput. .

  [04] Scanning of a single laser beam may be accomplished by a rotating mirror system or acousto-optic cell as disclosed in US Pat. No. 5,065,008. However, these single spot scanning architectures are inevitably limited in speed and can suffer from scanning aberrations, low illumination brightness, and potential thermal damage to the specimen when high brightness laser sources are used. is there. A stage-type scanning system is used that moves the specimen relative to a fixed illumination and image position while generating a synchronized scanning pattern by moving a single light spot over an area that is a fixed position. Even so, it is impossible to achieve the high data rates necessary to inspect the submicron structure of current semiconductor products.

  [05] Accordingly, there is a need for a sample scanning system that increases sample throughput while maintaining or even increasing the reliability and accuracy of data collected during sample scans, whether stationary or stage type systems. Has been. This demand utilizes multiple parallel scanning beams to scan the specimen, depending on whether the specimen is inspected by reflecting light from the surface or by transmitting light to the surface. It is satisfied by the present invention that by detecting multiple reflected or parallel transmitted beams and processing multiple reflected or transmitted beams simultaneously, the throughput is significantly increased over a single spot scanning system.

  [06] The present invention relates to a system for inspecting a specimen using a single light source that provides a light beam. The light beam is imaged by a moving lens acousto-optic device, which has an active region and selectively generates a plurality of moving lenses in the active region in response to the RF input signal. The moving lens acousto-optic device operates to receive a light beam and generate a plurality of spot beams at each of the focal points of the generated moving lens. The system also includes a photodetector unit that includes a plurality of detector sections, wherein each detector section operates to receive a plurality of photodetectors and inputs from the plurality of photodetectors in parallel. Two multi-stage storage devices. Information stored in each of the multi-stage storage devices is read continuously and continuously from a plurality of stages.

  [07] According to another feature of the invention, the invention includes a specimen inspection system that includes a plurality of scanning spot beam sources. The beam is imaged on the surface of the specimen, and multiple beams are generated by reflecting from or passing through the specimen. Optical detection having a plurality of detector sections, each detector section having a plurality of photodetectors and at least one multi-stage storage device operative to receive inputs from the plurality of photodetectors in parallel A unit is used. Information stored in each of the multi-stage storage devices is read continuously and continuously from a plurality of stages.

  [08] According to yet another aspect of the invention, the invention relates to a method for examining a specimen. This method includes providing a plurality of flying spots from a single light source and scanning a plurality of spot beams over the surface of the specimen so that the corresponding plurality of beams reflect off the specimen. Or by passing through the specimen. Thereafter, the contents of each of the reflected beams are captured and stored simultaneously in the respective signal storage sections. The stored information is continuously read, thereby increasing the speed and throughput of the scan data.

  [09] A further feature of the present invention is to achieve an acousto-optic device adapted to receive a light source and RF input to generate a plurality of moving lenses that provide a plurality of simultaneous scanning spots. This device has a crystal medium having an active region that defines a sound wave propagation direction, an RF chirp input, an RF input portion located at one end of the medium in the sound wave propagation direction, and a position intersecting the sound wave propagation direction. And includes a light input portion for receiving light from the light source and a light output portion. A series of RF pulses input to the RF input portion operate to generate a sequence of moving lenses that are simultaneously present in the active region, and the moving lens receives light input to the light input portion and from the light output portion. It operates to generate a plurality of output spot beams.

  [10] A further feature of the present invention is an RF input portion for generating a plurality of moving lenses having an active region, receiving a light source at the light input portion and providing a plurality of co-occurring spots from the light output portion. A method of operating an acousto-optic device adapted to receive. In this method, by inputting a series of chirp input pulses to the RF input portion, a sound wave is formed for each input pulse and propagates in the active region in the propagation direction, and in a direction crossing this propagation direction, Inputting light from a source into a light input portion and applying it to a sound wave propagating the light, the sound wave forming a moving lens and being simultaneously present in the active region, each moving lens comprising: By operating to focus and direct this light, a respective spot beam for each lens is output from the light output portion.

  [11] A further feature of the present invention is a linear photodetector unit for detecting a plurality of simultaneously scanned spot beams. The photodetector unit comprises a plurality of adjacent photodetector sections arranged linearly along a common axis. Each of the detector sections includes a plurality of adjacent photodetectors and at least one multi-unit that receives inputs from the plurality of photodetectors in parallel and operates to sequentially read information stored in the plurality of stages. And a stage storage device.

  [12] A further feature of the present invention is a method for detecting a plurality of pixels stored in a linear CCD having a first plurality of sections, each section comprising a second plurality of pixel storage elements. And receiving input from each of the third plurality of simultaneous scanning beams. The method includes capturing and storing the contents of each of the third plurality of beams simultaneously in respective signal storage sections and reading the stored signals simultaneously and continuously.

  [13] A further feature of the present invention is an apparatus for detecting both bright and dark field images from the surface of a specimen, wherein the bright field image is detected by at least one CCD, , Detected by at least one sensitive detector, such as a photomultiplier tube (PMT).

Detailed Description of the Invention

  [21] The following detailed description is exemplary embodiments of the invention, and the invention is not limited thereto, and modifications and auxiliary structures are known to those skilled in the art. May be added. In particular, but not as a limitation, with respect to inspecting a specimen surface by detecting reflected light using a light source and detection unit located on a common side of the specimen ("reflection system") Although embodiments are disclosed, those skilled in the art will detect a transmitted specimen by detecting transmitted light using a detection unit on the side of the specimen opposite to that of the light source (" It will be readily apparent that it is easily adaptable to a transmission system "). For example, the reflection system is different from the transmission system due to the absence of a beam splitter in the transmission system, but the principles of the present invention are applicable to both types of systems. As will be appreciated by those skilled in the art, both types of systems may be utilized separately or together when examining specimens according to the present invention.

  [22] FIG. 1 is a schematic diagram of a wafer, reticle, or similar specimen detection system 100 utilizing a moving lens multi-beam scanner according to the present invention. By way of example only, without limitation, the specimen may be any semiconductor product, such as an 8-inch or 12-inch wafer having multiple semiconductor elements, at any stage of several manufacturing stages, or It may be a mask, reticle, etc. used in the manufacturing process, and such specimens are indispensable for inspection with respect to defects, foreign matter, or pattern accuracy. In such a system, it is desirable to identify the size, position, and type of structures, defects, or objects that appear on the specimen surface with high accuracy and reliability. It is also desirable to speed up such identification in order to minimize manufacturing process delays that are subject to inspection and quality assurance steps.

  [23] The system 100 relies on a bright light source, such as a CW (or pulsed) laser 101, that generates a light beam output 151. Beam 151 is applied to a beamformer of conventional design that expands and collimates beam 151 to form beam 152 having a uniform intensity profile in a manner known to those skilled in the art. For wafer inspection, the laser operates at a short wavelength, such as 248 nm or 193 nm, for high resolution with stable output power (or stable pulse energy or pulse rate), stable transverse mode, and stable beam pointing. It is preferable to make it occur. The collimated beam 152 is applied to the conventional mirror 103 to form the beam 153 and direct it toward the working lens system, the components of which will be described in more detail below.

  [24] In particular, the formed beam 153 is projected onto a moving lens acousto-optic device 104 that operates to convert the formed beam 153 into a plurality of beams 154a, 154b, 154c. For convenience, three beams are illustratively shown, but the number of beams may be greater, and in the exemplary embodiment, there may be 10 or more simultaneously scanned beams. The moving lens acousto-optic device 104 responds to each of a series of chirped RF pulses, a single pulse produces a single lens, and the series of pulses causes the moving lens device 104 to have multiple graded lenses. It is formed. Each lens receives the input laser light and focuses it at the output to form the desired number of beams. As the RF pulse travels through the device 104, the associated lens moves to move each of those beams to the nature of the scan.

  [25] The basic theory, structure, and materials of acousto-optic cells are described in “Optical Scanning”, Gerald F., et al. Edited by Marshall, Chapter 11 (Marcel Dekker, Inc., 1991). As described on pages 675-677, single beam frequency chirp scanning involves acousto-optic Bragg cells to which a linear frequency sweep ("chirp") is applied. The frequency gradient generated at the optical aperture of the cell will act as a cylindrical lens whose focal length is based on a char plate. Light diffracted by the linearly swept acoustic frequency may converge or diverge and may be compensated by a complementary optical lens. According to this disclosure, acousto-optic scanners provide significant cost and performance advantages, and in particular random access times are short. Acousto-optic scanners typically produce a single scanning beam and, if multiple beams are desired, a plurality of chirp cells each receiving a chirp RF pulse, as disclosed on pages 682-83 of the Marshall book. Is required. More particularly, when a linearly increasing frequency is applied to each driver of each of the plurality of chirp cells in an array, successive angular scans of each collimated beam of the array are generated in response to Bragg conditions, resulting in time The creation of a phase grating with increasing pitch in the region results in a linear scan of the array of spots. With a high frequency cut-off, the driver signal is set to zero so that the chirp cell acoustic energy can be lost, resetting the spot before starting the next scan.

[26] Marshall, pages 682-683, teaches two types of acoustic array scanners, including those with doubled bandwidth and those with doubled resolution. In the first case, a large number of individually driven small closely spaced transducers are mounted in parallel on an acousto-optic medium made from TeO ₂ glass and PbMoO ₄ and TeO ₄ crystals. In the second case of the acousto-optic array, the components are arranged in series. An array of scanners, each having a specific resolution (number of points per line), can produce even higher resolution (number of points per line) by using composite optics.

[27] In contrast, the acousto-optic device 104 used in the present invention uses a single crystal that is effective in generating multiple moving lenses based on a series of input RF pulses. The device single crystal is preferably composed of a material compatible with a UV light source and has an acousto-optic medium made of fused silica, GaAs or TeO ₂ glass, but with compatibility with UV light. Other known materials may be used. The crystals have an anti-reflective coating on each major surface that is less than 0.5% on both sides. The device will operate in longitudinal acoustic mode at a center frequency of 200 MHz with a wavelength of 266 nm and a bandwidth of 130 MHz. The RF power is less than 3.0 watts. In one exemplary embodiment, the active aperture of the device may be “H” 1.0 mm × “L” 60 mm.

  [28] In operation, as shown in more detail in FIG. 4, laser light 401, which may be a single beam or a plurality of collimated beams, is converted into a Applied to one major surface 411. The RF generator 430 outputs a series of “chirp” or pulsed RF waveforms 431, 432, 433, etc. to an RF input port (SNA connector) 413, and in an exemplary embodiment, these durations and amplitudes are It is optimal that they are the same, but they may be different depending on the desired optical effect of the moving lens. The port is positioned transverse to the optical path, and an RF waveform can be injected at the edge of the crystal, and in an exemplary embodiment, at a speed that is approximately the same as 5.96 mm / μs or speed of sound. Establish a pressure wave across the length of. Pressure waves propagating through the crystal medium are aligned to provide stepped focus lenses 421, 422 to the laser light 401 entering the input major surface 411 and exiting the output major surface 412. As will be appreciated by those skilled in the art, each lens 421, 422 will focus the passing beams 441, 442 at focal points 443, 444.

  [29] Referring again to FIG. 1, the effect of creating a plurality of graded lenses 104a, 104b, 104c in the active region of the acousto-optic device 104 is that of the moving lens acousto-optic device for each of the created lenses. Flying spots are generated at the focal points 154a, 154b, 154c. Thereafter, the flying spots 154a, 154b, 154c pass through the conventional collimator lens 105, and the collimated beams 155a, 155b, 155c are incident on the surface 106a of the dichroic mirror 106, but the dichroic mirror 106 pass. The mirror 106 provides all of the collimated beams 155a, 155b, 155c to the objective lens 107 for imaging as a plurality of beams 156a, 156b, 156c on the surface of the scanned wafer, reticle, or other specimen 108. send. A plurality of parallel beams 156a, 156b, 156c output by the objective lens 107 are focused on individual spots 108a, 108b, 108c on the surface of a wafer, reticle, or other specimen, and the parallel beams 157a, 157b, Reflected as 157c. These reflected beams 157a, 157b, and 157c pass through the objective lens 107 again and are directed to the back surface 106b of the dichroic mirror 106. These parallel reflected beams 158 a, 158 b and 158 c are reflected by the mirror 106 and applied to the collimator lens 109.

  [30] The beam from the lens 109 is output to a camera having a multi-stage, multi-tap vertical transfer CCD 110. The CCD has a respective detection area 111, 112, 113 illuminated by one of the beams 159a, 159b and 159c. As the beam scans the surface of the wafer 108 and generates a parallel image stream, the cells in each sector 111, 112, 113 of the charge coupled device 110 capture an output pixel in each of each beam. Each sector 111, 112, 113 of the multi-tap CCD 110 has shift register sections 114, 115, 116 corresponding to the beams 159a, 159b, 159c, respectively. These parallel input sectors may be read in parallel, increasing the throughput of the image detection device. Thus, in a given time period, a series of read pulses are input to each of the shift registers to perform parallel reads, thereby outputting their contents in a parallel data stream.

  [31] In a general example, the first sector 111 having the shift register 114 is read by the sector transfer signal 160 a input through the amplifier 121. This signal is a series of pulses that cause a shift register with stages mounted in parallel to read data continuously to the output line 161a via the buffer 131. Similarly, the clocking signals of sector 2 and sector 3 are applied to shift registers 115 and 116 of multi-tap CCD sectors 112 and 113 via amplifiers 122 and 123, respectively. The resulting data, read continuously through amplifiers 132, 133, is provided to data outputs 161b, 161c.

  [32] Taking a light beam 157a, 157b, 157c back-reflected from the surface of the wafer or specimen 108 by a multi-section tap linear CCD structure 110 provides a highly effective and efficient design. Structure 110 is constructed such that the same objective lens structure is used for scanning and reflected light. Furthermore, when the reflected light from each scanning beam is applied to the segmented CCD structure 110, the content of the information derived from scanning each section of the specimen is transferred in parallel to a temporary shift register. Are read continuously. Transfer from multiple sectors of the CCD 110 provides a large amount of data throughput, which is highly desirable in a wafer inspection system.

[01] FIG. 5 illustrates an exemplary embodiment of a sensor 500 with a practical camera design. The device is a linear CCD having 2048 elements 501, each element having a horizontal dimension of 16 μm, a vertical dimension of 64 μm, and a pixel pitch of 16 μm. The 2048 elements are divided into 64 independent sections 502 each having 32 elements 501, each element 501 having an output 503 to a first temporary storage stage 504, this output 503 is provided in parallel with the outputs of the other 31 elements of section 502. Section 502 is located immediately adjacent to another section. In another embodiment, 128 outputs may be provided with only 16 pixels per tap for speed. The 32 values of each first temporary storage stage 504 are read in parallel to the respective second stage storage stage 505 by the respective clocks C ₁ -C ₆₄ and stored in all second stage storages. 32 values of the stage 505, in response to a single clock C _0, are read into the respective read shift register stage 506. 32 bytes of each read shift register stage 506 is clocked continuously by clock input _{C K,} voltage mode, which is the analog output from the register, the respective output ports _OUT 1 to OUT ₆₄ for each of the 64 sections 502 Given. As will be appreciated by those skilled in the art, an appropriate voltage is applied to the device for proper operation. Sensors with this architecture may be designed to have a data rate of 20-40 MHz (1.0-1.6 MHz line rate) and an output in the range of 2.0-3.2 Gpix per second.

  [34] Returning again to the schematic of FIG. 1, the spot timing is designed so that there is only one spot for a single CCD section 114-116. In fact, in the exemplary embodiment using the linear sensor of FIG. 5 and a 10 beam scanner, only one sixth of the 64 sensor segments, each with storage for 32 pixels, receive one input at a time. become. Entering a single beam into multiple segments provides a delay that allows the necessary storage and readout processing as the beam moves to the next section. By way of example and not limitation, FIG. 2 shows a timing diagram for only two spots, but may be easily estimated for additional spots with the following teachings. In the figure, a timing (t) line 200 provides a reference for scanning a wafer surface, reticle, or other surface by a plurality of spots. While the surface moves in the y (page length) direction at a predetermined speed, the spot scans along the x (page width) direction. Initially, spot 1 is placed on section 1 of the wafer and scans through section 1 of the wafer or other surface, as shown at position 211 during time period 201. The scan is tilted upward to the right side by upward movement of the surface due to movement of the wafer or the like on the stage. The second spot has not yet been scanned, as shown at processing position 220. Since only the first spot is scanned during time period 201, there is no data transferred from section 1 in processing section 230 or section 2 in processing section 230 and no data output in processing section 250.

  [35] During the second time period 202, the scan of section 1 is completed by spot 1 and begins the scan of section 2, as indicated by the portion of scan line 212. At the same time, the second spot begins scanning section 1 as indicated by scan line 221. At the start of time period 202, all of the data acquired during the section 1 scan in period 201 is output in parallel at 231. However, since there is no data stored for section 2 at this time, there is no input at processing portion 240. However, the data transferred in parallel from section 1 at 231 is continuously output during time period 202 as indicated by output 251 of data section 1.

  [36] At the beginning of period 203, spot beam 1 begins scanning section 3 at 213, while spot beam 2 begins scanning section 2 at 222. In the processing portion 230, the data accumulated by spot 2 in section 1 is transferred at 232, whereas the data at spot 1 in section 2 is transferred at 241. During time period 203, the data for each of sections 1 and 2 (collected by scans 221, 212) is read continuously at 252 and 253, respectively. For an exemplary embodiment using 10 beams and having 64 sections of a linear scanner, return at least 6 sections of the CCD to the start of another scan after receiving input from each beam. Obviously, the beam must scan a portion of the surface, such as a wafer. Therefore, there is a delay in data output corresponding to the scanning of six sections. Synchronization between beam scanning and CCD output is easily achieved to achieve optimum output.

  [37] FIG. 3 shows an actual surface 300 of a wafer, reticle, or similar object under inspection. Horizontal scales 0-12 identify the location of individual pixels (bright squares 301-312), and some of these pixels (301, 304, 307, and 310) may be on wafers, reticles, or other This is the scanning start point of scanning that proceeds in a direction orthogonal to the movement of the object. This movement is in the direction marked by the numbers 0-10. The wafer itself is scanned by multiple beams 350, 360, and 370 in a single series, and the beam scan is repeated in subsequent series, as shown at the start of scan series 350 ′ at pixel 10 on the right side of the figure. It is. As the wafer is moved by a conventional transfer stage apparatus 170 (FIG. 1), indicated by the progression of the numbers 0-10 in the vertical direction, the beam appears to scan diagonally across the surface of the wafer. Therefore, in the first series scan, the spot 350 starts at the point 301 in the sector 1. Thereafter, as it scans, spot 350 moves to pixel 302 in sector 2, pixel 303 in sector 3, and so on. The second spot 360 begins at point 304 in sector 1, moves to point 305 in sector 2, point 306 in sector 3, point 307 in sector 4, and so on. A spot 370 starting at point 7 in sector 1 moves similarly. The second series of scans begins again at spot 350 ′, but in this case begins at point 310 in sector 1. In the second scan, the scans of spots 360 and 370 are similarly repeated, and as the wafer is moved by stage 170, the scans of spots 350-370 are similarly repeated in subsequent series. By performing this scanning, the parallel readout values of the entire area of the wafer can be viewed.

  [38] A second exemplary embodiment is shown in FIG. 6A, in which the system 600 is substantially the same as the embodiment of FIG. The difference is that a beam splitter is used to create the beam. More particularly, the laser 601 generates a light beam output 651 that is applied to a conventional beamformer 602 to form a beam 652 having a uniform intensity beam profile in a manner known to those skilled in the art. The collimated beam 652 is applied to a conventional mirror 603 for directing the beam 653 to a working lens system having an acousto-optic moving lens 604. The moving lens acousto-optic device 604 operates to convert the formed beam 653 into a plurality of beams 654a, 654b, 654c. Again, for convenience, three beams are illustratively shown, but the number of beams may be greater, and in the exemplary embodiment, with ten or more simultaneous scanning beams. It may be. Moving lens acousto-optic device 604 is responsive to each of a series of chirped RF pulses to form one of a plurality of graded lenses in the active region of moving lens device 604. As the acoustic pulse travels through device 604, the associated lens transitions and moves each of those beams to the nature of the scan. A plurality of graded lenses 604a, 604b, 604c in the active region of the acousto-optic device 604 generate a plurality of flying spots at the focal point 654a, 654b, 654c of the moving lens acousto-optic device, and then the flying spots 654a, 654b. , 654c passes through a conventional collimator lens 605.

[39] Unlike the first embodiment, the multiple beam output of the collimator lens 605 is a Dammam grating or beam splitter (1 × 3 type in the illustrated embodiment, but other split ratios are within the scope of the present invention. ) Produces several spread beams 655a, 655b, 655c. The splitting may be performed by any means known to those skilled in the art as long as the energy of each split beam is substantially equal. Each of these beams is incident on the surface of the dichroic mirror 606 and is applied to an objective lens 607 for imaging the surface of the sample 608 _to be scanned as a plurality of beams 656a _{1 to 3} , 656b ₁ to ₃ , and 656c _{1 to 3} . A plurality of spot beams (655a _{1 to 3} , 655b _{1 to 3} , 655c _{1 to 3} , not shown) to be passed are included. The plurality of parallel beams 656a _1-3 , 656b _1-3 , 656c _1-3 output by the objective lens 607 are focused on regions 608a, 608b, 608c on the surface of the specimen. Each of these regions is scanned by a separate flying spot resulting from a separate one of the beams 655a, 655b, and 655c, which in the exemplary embodiment generates a scan line structure as shown in FIG. in a separate beam 656a _2, 656b _2, scanning from 656c ₂ is an unity, it is out of time and position. These scans are returned as parallel beams (three beams in each of the three scans, not shown), and these beams pass again through the objective lens 607 and are directed to the back of the dichroic mirror 606. These parallel reflected beams are reflected by the mirror 606 and applied to the collimator lens 609.

[40] Beams 659a _1-3 , 659b _1-3 , 659c _1-3 from the lens 609 are output to three cameras, each of which is similar to that of the linear CCD of the embodiment of FIG. Multi-stage and multi-tap vertical transfer CCDs 610A, 610B, and 610C each having the structure and function described above are provided. This architecture further increases the throughput and resolution of the image detection device.

  [41] In yet another exemplary embodiment, as shown in FIG. 7a, laser light from a light source that may include multiple flying spots or a single spot as previously disclosed, It may pass through the dichroic mirror 710. The mirror 706 allows the laser light 701 to pass through the first surface 710a, but reflects light returning from the specimen from the opposite surface 710b. The passed laser light 702 passes through a second dichroic mirror having a first surface 720 a that allows the laser light to pass therethrough and a second surface 720 b that reflects the dark field light 704. Laser light 703 that collides with the surface of the specimen 708 is reflected back as dark field light 704 and bright field light 705. The dark field light 704 is separated from the bright field light 705 by the surface 720b of the annular mirror 720 that reflects the dark field light and passes the bright field light. Dark field light 704 is detected by a highly sensitive photomultiplier tube (PMT) 740. PMTs of conventional design and commercially available from manufacturers Hammatsu and Burle are particularly beneficial when there is dark field low light scattering. The bright field light is reflected through the mirror 720 by the surface 710b to the CCD 730, which may be a multistage or single stage CCD, with lower sensitivity but greater dynamic range than PMT. It is fast.

  [42] In another embodiment, the dichroic mirror 760 and the dichroic mirror 770 are advanced to an objective lens 757 for focusing on the surface of the specimen 758, and by a moving lens according to the principles already disclosed herein. A laser 751 in the form of an annular illumination that may be scanned is provided. The reflected light, which is a dark field and bright field component, is directed to the surface of the mirror 770, and the bright field light is reflected toward the CCD 790. The dark field light passes through the mirror 770 to the mirror 760, and the surface of the mirror reflects the light to the PMT 780 for detection.

  [43] Although the invention has been described with reference to several exemplary embodiments, the invention is not limited thereto, and the full scope of the invention is intended to be construed in accordance with applicable law. In the following claims.

1 shows a schematic diagram of a first exemplary system and apparatus for scanning a wafer or other specimen according to the present invention. FIG. 4 shows an exemplary timing diagram for using multiple beams generated by the apparatus of the present invention to scan a wafer or other specimen. Fig. 4 shows a topography of the wafer surface when scanned simultaneously by four beams generated according to an embodiment of the present invention. 1 is a schematic diagram of a moving lens, multi-beam acousto-optic device when used in one embodiment of the present invention. 1 is a schematic diagram of a multi-stage linear photodiode with two-stage vertical transfer that may be used in a CCD scanner according to one embodiment of the present invention. 2 is a schematic diagram of a second exemplary system and apparatus for scanning multiple split beams on a wafer or other specimen according to the present invention. 2 is a schematic diagram of a line structure scanned against a split beam according to the present invention. 1 is a schematic illustration of a single illumination laser architecture for separately detecting bright and dark field images on a specimen surface. 1 is a schematic illustration of an annular illumination laser architecture for separately detecting bright and dark field images on a specimen surface.

DESCRIPTION OF SYMBOLS 100 ... Wafer detection system, 101 ... Laser, 102 ... Beam former, 103 ... Mirror, 104 ... Moving lens acousto-optic device, 106 ... Dichroic mirror, 107 ... Objective lens, 108 ... Wafer, 109 ... Collimator lens, 110 ... Vertical Transfer CCD, 114... Shift register.

Claims (7)

A linear photodetector device for detecting a plurality of simultaneously scanned spot beams,
Comprising a plurality of adjacent light detector section located linearly along a common axis, each photodetector section that is arranged to detect individually the scanning spot beam,
A plurality of adjacent photodetectors;
Receiving an input from said plurality of photodetectors in parallel, and a least one multi-stage storage device operates to the information stored in the multi-stage storage device are read out continuously in a series of pulses ,
The multi-stage storage device of the plurality of adjacent photodetector sections outputs the information to simultaneously read in parallel in a series of pulses of the information ;
Linear photodetector.   The linear photodetector of claim 1, wherein each photodetector section comprises an input for a section transfer signal. So that the each optical detector section, comprises a temporary shift register having a plurality of stages, the shift register is received at each stage the contents of the corresponding detector in parallel, are read sequentially in a series of pulses The linear photodetector according to claim 2, wherein the linear photodetector operates. Buffer To further comprising a section transfer signal source, the signal source supplies a section transfer signal to continuously read a plurality of said stages, conveying the signal read continuously in a series of pulses The linear detector of claim 3 , providing a data output line comprising: A method for detecting a plurality of pixels stored in a linear photodetector according to claim 1 , comprising:
Receiving, in parallel, inputs from each of a plurality of simultaneous scanning beams at the plurality of photodetectors in each of the photodetector sections;
In each of the multi-stage storage devices of the photodetector section, a step of simultaneously captures stores each signal of said plurality of simultaneous scanning beam,
It said plurality of said multi-stage storage device adjacent photodetector section, outputs the signal stored in the multi-stage storage device from the plurality of photodetectors section continuously simultaneously a series of pulses in parallel Steps,
Including a method. 6. The method of claim 5, further comprising synchronizing the timing of scanning of the plurality of simultaneous scanning beams and the timing of reading of the signal. Wherein the step of incorporation storing are performed simultaneously in only a portion of the plurality of photodetectors section The method of claim 5.

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